Shankar Exercise 2.5.1 - Hamiltonion

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Homework Statement



Could someone get me started with Exercise 2.5.1 in Shankar's Principles of Quantum Mechanics?
Does this forum support TeX or LaTeX?


Homework Equations






The Attempt at a Solution

 
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Post the text of the problem for those of us who don't have the book, but might be willing to help you.
 
Ad 2: Yes, use the [ tex] tag (without the space):
\left[-\frac{\hbar^2}{2 m} \nabla^2 + U(\mathbf{r}) \right] \psi (\mathbf{r}) = E \psi (\mathbf{r}).
 
Show that if T = \sum_i\sum_jT_ij(q)q_i' q_j', where q_i''s are generalized velocities, then \sum p_i q_i' = 2T.
 
And was does the rest stand for?

Work done so far? etc.
 
T is kinetic energy and pi is the canonical momentum conjugate. Also, the apostrophes are derivatives. Sorry.

There is not much work done so far. I wanted someone to give me a hint or just get me started.
 
By the way, does anyone have Shankar's book? For a lot of his exercises you really need the context, so I want to know if I should keep posting questions from his book.
 
ehrenfest said:
Show that if T = \sum_i\sum_jT_ij(q)q_i' q_j', where q_i''s are generalized velocities, then \sum p_i q_i' = 2T.

Since p_{i}=\frac{\partial L}{\partial q^{i}}, i gues the result is pretty obvious, don't you think ?
 

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